Add riding eps example
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@ -51,6 +51,7 @@ def __calc_chi(mode='density'):
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lastkurt=None
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lastkurt=None
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for dim in dims:
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for dim in dims:
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try:
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try:
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1/0
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with open(path+f"magnets/magnetisation_{mode}_dim={dim:02}.txt", 'r', encoding='utf-8') as f:
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with open(path+f"magnets/magnetisation_{mode}_dim={dim:02}.txt", 'r', encoding='utf-8') as f:
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magnet = json.load(f)
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magnet = json.load(f)
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with open(path+f"suscepts/susceptibility_{mode}_dim={dim:02}.txt", 'r', encoding='utf-8') as f:
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with open(path+f"suscepts/susceptibility_{mode}_dim={dim:02}.txt", 'r', encoding='utf-8') as f:
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@ -87,7 +88,7 @@ def __calc_chi(mode='density'):
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else:
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else:
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raise NotImplementedError
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raise NotImplementedError
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mag = round(abs(mag),6)
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mag = round(abs(dmag),6)
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fluct = round(mag2-mag**2,6)
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fluct = round(mag2-mag**2,6)
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tail = round(mag4/mag2**2,6)
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tail = round(mag4/mag2**2,6)
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71
evaluation/2Layer Sonic.py
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71
evaluation/2Layer Sonic.py
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@ -0,0 +1,71 @@
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# -*- coding: utf-8 -*-
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"""
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Created on Tue Aug 30 14:25:12 2022
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@author: timof
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"""
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import sys
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import os
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import json
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# from plot import qtplot
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from scipy.io import wavfile
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import math as m
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import numpy as np
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vect = np.vectorize
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@vect
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def log2(x):
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try:
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return m.log2(x)
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except ValueError:
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if x==0:
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return float(0)
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else:
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raise
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def new_folder(path):
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if not os.path.exists(path):
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os.makedirs(path)
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return path
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phase = np.vectorize(lambda x,y: (m.atan2(y,x)+m.pi)%(2*m.pi)-m.pi)
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diff = np.vectorize(lambda x,y: (y-x+m.pi)%(2*m.pi)-m.pi)
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H2 = lambda x: -x*m.log2(x)-(1-x)*m.log2(1-x)
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path = '/cloud/Public/_data/neuropercolation/2lay/steps=500000_rising/'
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suffix = ''
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chi = chr(967)
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vareps = chr(949)
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vals = [[],[]]
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runsteps = 1000100
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eps_space = np.linspace(0.005, 0.5, 100)
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eps_space = eps_space[1::2]
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dims = [121]#+[16,49]
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mode='density'
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ma=[]
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s=[]
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k=[]
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mk=[]
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lastkurt=None
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for dim in dims:
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dimpath = new_folder(path + f'dim={dim:03d}/')
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for epsilon in [0.000]:
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with open(dimpath+f"eps={round(epsilon,3):.3f}_activation.txt", 'r', encoding='utf-8') as f:
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activation = np.array(json.load(f)[::-1])
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# activation = list(zip(*activation))
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wavfile.write(dimpath+f"eps={round(epsilon,3):.3f}_activation_48k.wav_rev",48000,activation)
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@ -345,13 +345,13 @@ qtplot(f'Q facor for odd automaton sizes',
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# FWHM=json.load(f)
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# FWHM=json.load(f)
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qtplot(f'Dominant frequency',
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qtplot(f'Dominant frequency',
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[[0]+list(eps_space[:-1])]*3,
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[[0]+list(eps_space[:20])]*3,
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[[0]+FMAX[-1],[0]+LHM[-1],[0]+UHM[-1]],
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[[0]+FMAX[:20],[0]+LHM[:20],[0]+UHM[:20]],
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# [f'dim={dim}x{dim}' for dim in dims],
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# [f'dim={dim}x{dim}' for dim in dims],
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['dominant frequency', 'lesser half maximum', 'upper half maximum'],
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['FMAX', 'FMAX-FWHM/2', 'FMAX+FWHM/2'],
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#colors=['g','r','r'],
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colors=['r','r','g'],
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y_tag = 'frequency f',
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y_tag = 'frequency f',
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y_log = True,
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y_log = False,
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export=True,
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export=True,
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path=sigpath,
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path=sigpath,
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filename=f'FMAX+FWHMto50_plot_{parts}parts_accum={accum}.png',
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filename=f'FMAX+FWHMto50_plot_{parts}parts_accum={accum}.png',
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@ -89,6 +89,7 @@ qtplot(f"Mean effect integration over noise level",
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[[0]+phi for phi in PHI[::-1]],
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[[0]+phi for phi in PHI[::-1]],
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[f'dim={dim:02d}x{dim:02d}' for dim in dims[::-1]],
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[f'dim={dim:02d}x{dim:02d}' for dim in dims[::-1]],
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y_tag = f'effect integration {varphi}',
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y_tag = f'effect integration {varphi}',
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x_tag = f'noise level {vareps}',
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export=True,
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export=True,
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path=dimpath+"",
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path=dimpath+"",
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filename=f'eps={round(epsilon,3):.3f}_evolution.png',
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filename=f'eps={round(epsilon,3):.3f}_evolution.png',
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77
evaluation/4Layer Sonic.py
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77
evaluation/4Layer Sonic.py
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@ -0,0 +1,77 @@
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# -*- coding: utf-8 -*-
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"""
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Created on Tue Aug 30 14:25:12 2022
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@author: timof
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"""
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import sys
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import os
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import json
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from plot import qtplot
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import math as m
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import numpy as np
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vect = np.vectorize
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@vect
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def log2(x):
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try:
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return m.log2(x)
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except ValueError:
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if x==0:
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return float(0)
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else:
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raise
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def new_folder(path):
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if not os.path.exists(path):
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os.makedirs(path)
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return path
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path = '/cloud/Public/_data/neuropercolation/4lay/cons=27-knight_steps=100100_causal/dim=09/batch=0/'
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suffix = ''
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chi = chr(967)
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vareps = chr(949)
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vals = [[],[]]
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runsteps = 1000100
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eps_space = np.linspace(0.005, 0.5, 100)
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eps_space = eps_space[1::2]
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dims = list(range(3,10))#+[16,49]
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mode='density'
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ma=[]
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s=[]
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k=[]
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mk=[]
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lastkurt=None
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for dim in dims[-1:]:
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dimpath = new_folder(path + f'dim={dim:02}/')
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for epsilon in eps_space[:]:
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with open(path+f"eps={round(epsilon,3):.3f}_phase_diff.txt", 'r', encoding='utf-8') as f:
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phase_diff = np.array(json.load(f)[:500])
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with open(path+f"eps={round(epsilon,3):.3f}_ei.txt", 'r', encoding='utf-8') as f:
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phase_diff = np.array(json.load(f)[:500])
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qtplot(f"Phase relation time series for eps={round(epsilon,3):.3f}",
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[list(range(500))]*2,
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[phase_diff],
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x_tag = 'time step',
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y_tag = f'phase diffe´rence',
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y_range = (-m.pi,m.pi),
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export=True,
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path=dimpath+"evolution/",
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filename=f'eps={round(epsilon,3):.3f}_evolution.png',
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close=False)
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mode = 'density'
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#%%
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@ -71,20 +71,20 @@ for _eps in _epses[11:21]:
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# sign_p_list.append(sign_p)
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# sign_p_list.append(sign_p)
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# with open(savepath+f"phasediff_means.txt", 'w', encoding='utf-8') as f:
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with open(savepath+f"phasediff_means.txt", 'w', encoding='utf-8') as f:
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# json.dump(meanlist, f, indent=1)
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json.dump(meanlist, f, indent=1)
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# with open(savepath+f"phasediff_stds.txt", 'w', encoding='utf-8') as f:
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with open(savepath+f"phasediff_stds.txt", 'w', encoding='utf-8') as f:
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# json.dump(stdlist, f, indent=1)
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json.dump(stdlist, f, indent=1)
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# with open(savepath+f"phasediff_integrals.txt", 'w', encoding='utf-8') as f:
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with open(savepath+f"phasediff_integrals.txt", 'w', encoding='utf-8') as f:
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# json.dump(integrallist, f, indent=1)
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json.dump(integrallist, f, indent=1)
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# with open(savepath+f"phasediff_cohends.txt", 'w', encoding='utf-8') as f:
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with open(savepath+f"phasediff_cohends.txt", 'w', encoding='utf-8') as f:
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# json.dump(cohendlist, f, indent=1)
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json.dump(cohendlist, f, indent=1)
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# with open(savepath+f"phasediff_norm_ps.txt", 'w', encoding='utf-8') as f:
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with open(savepath+f"phasediff_norm_ps.txt", 'w', encoding='utf-8') as f:
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# json.dump(norm_p_list, f, indent=1)
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json.dump(norm_p_list, f, indent=1)
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# with open(savepath+f"phasediff_ttest_ps.txt", 'w', encoding='utf-8') as f:
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with open(savepath+f"phasediff_ttest_ps.txt", 'w', encoding='utf-8') as f:
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# json.dump(ttest_p_list, f, indent=1)
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json.dump(ttest_p_list, f, indent=1)
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# with open(savepath+f"phasediff_sign_ps.txt", 'w', encoding='utf-8') as f:
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with open(savepath+f"phasediff_sign_ps.txt", 'w', encoding='utf-8') as f:
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# json.dump(sign_p_list, f, indent=1)
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json.dump(sign_p_list, f, indent=1)
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# stdlowlist = [meanlist[eps] - stdlist[eps] for eps in range(len(meanlist))]
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# stdlowlist = [meanlist[eps] - stdlist[eps] for eps in range(len(meanlist))]
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# stdhighlist = [meanlist[eps] + stdlist[eps] for eps in range(len(meanlist))]
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# stdhighlist = [meanlist[eps] + stdlist[eps] for eps in range(len(meanlist))]
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@ -105,19 +105,19 @@ for _eps in _epses[11:21]:
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filename=f'Resultant reduction disconnect eps={_eps} dim={_dim} extremes={_ext}.png',
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filename=f'Resultant reduction disconnect eps={_eps} dim={_dim} extremes={_ext}.png',
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close=True)
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close=True)
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# qtplot(f'Mean causal phase reduction for dt={_dt} dim={_dim} with 4 layers',
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qtplot(f'Mean causal phase reduction for dt={_dt} dim={_dim} with 4 layers',
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# [_epsilons]*3,
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[_epsilons]*3,
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# [stdlowlist, stdhighlist, meanlist],
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[stdlowlist, stdhighlist, meanlist],
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# ['Low standard deviation',
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['Low standard deviation',
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# 'High standard deviation',
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'High standard deviation',
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# 'Mean'],
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'Mean'],
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# colors=['r','r','g'],
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colors=['r','r','g'],
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# x_tag = f'noise level {chr(949)}',
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x_tag = f'noise level {chr(949)}',
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# y_tag = 'abs phase reduction',
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y_tag = 'abs phase reduction',
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# export=True,
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export=True,
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# path=savepath,
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path=savepath,
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# filename=f'Mean phase reduction dim={_dim} extremes={_ext}.png',
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filename=f'Mean phase reduction dim={_dim} extremes={_ext}.png',
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# close=True)
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close=True)
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# qtplot(f'Phase reduction probability for dt={_dt} dim={_dim} with 4 layers',
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# qtplot(f'Phase reduction probability for dt={_dt} dim={_dim} with 4 layers',
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# [_epsilons],
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# [_epsilons],
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# [integrallist],
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# [integrallist],
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from datetime import datetime
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from datetime import datetime
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from random import sample as choose
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from random import sample as choose
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from random import random
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from random import random
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from numba import jit, njit, prange
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import itertools
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#from numba import jit, njit, prange
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from plot import qtplot
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# from plot import qtplot
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from neuropercolation import Simulate4Layers
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# from neuropercolation import Simulate4Layers
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eps_space = list(np.linspace(0.01,0.2,20))
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eps_space = list(np.linspace(0.01,0.2,20))
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def new_folder(path):
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def new_folder(path):
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@ -29,7 +30,7 @@ phase = np.vectorize(lambda x,y: (m.atan2(y,x)+m.pi)%(2*m.pi)-m.pi)
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diff = np.vectorize(lambda x,y: (y-x+m.pi)%(2*m.pi)-m.pi)
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diff = np.vectorize(lambda x,y: (y-x+m.pi)%(2*m.pi)-m.pi)
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H2 = lambda x: -x*m.log2(x)-(1-x)*m.log2(1-x)
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H2 = lambda x: -x*m.log2(x)-(1-x)*m.log2(1-x)
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@njit
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def neighbor(digit0, digit1, lenght):
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def neighbor(digit0, digit1, lenght):
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layer = int(lenght)
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layer = int(lenght)
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dim = int(np.sqrt(layer))
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dim = int(np.sqrt(layer))
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else:
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else:
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return False
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return False
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@njit
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def kcomb(zp,zm):
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def kcomb(zp,zm):
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if zp>2:
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if zp+zm>5:
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val=None
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elif zp>2:
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val=1
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val=1
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elif zm>2:
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elif zm>2:
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val=0
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val=0
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else:
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else:
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raise NotImplementedError(zp,zm)
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raise NotImplementedError(zp,zm)
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return val
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return val
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#%%
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neighbourcomb = [[(i,j) for j in range(6)] for i in range(6)]
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probcombs = [[kcomb(*n) for n in row] for row in neighbourcomb]
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posscombs = {val for row in probcombs for val in row}
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probcombs1 = [kcomb(n,4-n) for n in range(5)]
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eta = lambda eps: 1-eps
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etastar = lambda eps,kp: kp*(1-eps)+(1-kp)*eps
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epsstar = lambda eps,kp: kp*eps+(1-kp)*(1-eps)
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KL = lambda eps,kp: eta(eps)*m.log2(eta(eps)/etastar(eps,kp)) + eps*m.log2(eps/epsstar(eps,kp)) if kp is not None else 0
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phi_mat = lambda eps: [[KL(eps,kcomb(i,j)) for j in range(6)] for i in range(6)]
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phi_vals = lambda eps,df=4: sorted({sum([KL(eps,kp) for kp in kps]) for kps in itertools.product(*[[1,0.5]]*df)})
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phi_sing = lambda eps: KL(eps,kcomb(1,0))
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phi_lims = lambda eps: [phi_sing(eps)+val for val in phi_vals(eps)]
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#%%
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path = new_folder('/cloud/Public/_data/neuropercolation/1lay/mips/')
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path = new_folder('/cloud/Public/_data/neuropercolation/1lay/mips/')
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@ -125,22 +145,29 @@ def MIP(dim,statestr,eps):
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return mip,lophi
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return mip,lophi
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def calc_mips(dim,eps):
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def calc_mips(dim,eps,save=True):
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mip = []
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mips = [[] for i in range(5)]
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statestr='0'*dim**2
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statestr='0'*dim**2
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lims = phi_lims(eps)
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# statestr=statestr.translate(str.maketrans('','','.-='))
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# statestr=statestr.translate(str.maketrans('','','.-='))
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for parti in range(1,2**(dim**2-1)):
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for parti in range(1,2**(dim**2-1)):
|
||||||
partstr = bin(parti)[2:].zfill(dim**2)
|
partstr = bin(parti)[2:].zfill(dim**2)
|
||||||
curphi = phi(dim,statestr,partstr,eps)
|
curphi = phi(dim,statestr,partstr,eps)
|
||||||
mip.append(round(curphi,6))
|
for cha,mip in enumerate(mips):
|
||||||
|
if curphi<lims[cha]:
|
||||||
|
mip.append(parti)
|
||||||
|
print(f'Part {partstr} in mips[{cha}] with phi={curphi}')
|
||||||
|
|
||||||
mipath = new_folder(path+f'dim={dim:02d}/')
|
mipath = new_folder(path+f'dim={dim:02d}/')
|
||||||
with open(mipath+f"eps={round(eps,3):.3f}_mips.txt", 'w', encoding='utf-8') as f:
|
for cha,mip in enumerate(mips):
|
||||||
json.dump(mip, f, indent=1)
|
with open(mipath+f"eps={round(eps,3):.3f}_mipis_{cha}.txt", 'w', encoding='utf-8') as f:
|
||||||
|
json.dump(mip, f, indent=1) if save else None
|
||||||
|
return mips
|
||||||
|
|
||||||
def smartMIP(dim,statestr,eps):
|
def smartMIP(dim,statestr,eps):
|
||||||
lophi=np.inf
|
lophi=np.inf
|
||||||
mip = []
|
mip = []
|
||||||
|
phi_lims = phi_vals(eps)
|
||||||
|
|
||||||
for parti in range(0,dim**2):
|
for parti in range(0,dim**2):
|
||||||
partstr = bin(2**parti)[2:].zfill(dim**2)
|
partstr = bin(2**parti)[2:].zfill(dim**2)
|
||||||
|
@ -23,7 +23,8 @@ for eps in eps_ep:
|
|||||||
boots.append(ps)
|
boots.append(ps)
|
||||||
|
|
||||||
|
|
||||||
|
lower=[0.001]*len(ps)
|
||||||
|
higher=[0.999]*len(ps)
|
||||||
|
|
||||||
|
|
||||||
|
qtplot(f"Bootstrapping p-value for noise level {eps}",[range(dt+1)]*3,[lower,higher,ps],[f'right-sided p-value','p=0.999 limit','p=0.001 limit'],colors=['w','r','g'],y_tag='p-value',y_log=False)
|
||||||
qtplot(f"Bootstrapping p-value for noise level {eps}",[range(dt+1)],boots[-1:],[f''],y_tag='p-value',y_log=False)
|
|
25
evaluation/plots/significance_plot.py
Normal file
25
evaluation/plots/significance_plot.py
Normal file
@ -0,0 +1,25 @@
|
|||||||
|
from plot import qtplot
|
||||||
|
import json
|
||||||
|
import math as ma
|
||||||
|
import numpy as np
|
||||||
|
|
||||||
|
path='/cloud/Public/_data/neuropercolation/4lay/cons=27-knight_steps=1000100_diares/dim=09/batch=0/allpos_ei_samples=10000/dt=1/'
|
||||||
|
eps_sp=np.linspace(0.005,0.2,40)
|
||||||
|
eps_ep=eps_sp
|
||||||
|
|
||||||
|
extremes=10000
|
||||||
|
strength=100000
|
||||||
|
|
||||||
|
savepath=path+f'extremes={extremes}_bootstrength={strength}/'
|
||||||
|
|
||||||
|
with open(path+f"phasediff_means.txt", 'r', encoding='utf-8') as f:
|
||||||
|
means=json.load(f)
|
||||||
|
with open(path+f"phasediff_stds.txt", 'r', encoding='utf-8') as f:
|
||||||
|
stds=json.load(f)
|
||||||
|
|
||||||
|
|
||||||
|
hirim=[means[i]+stds[i] for i in range(len(means))]
|
||||||
|
lorim=[means[i]-stds[i] for i in range(len(means))]
|
||||||
|
|
||||||
|
|
||||||
|
qtplot(f'Reduction of phase deviation to noise level',[[0]+list(eps_sp[:40])]*3,[[0]+lorim,[0]+means,[0]+hirim],['mean-std','mean','mean+std'],colors=['r','g','r'],y_tag='phase difference',y_log=False)
|
29
examples/Simulate2Layers rising eps.py
Normal file
29
examples/Simulate2Layers rising eps.py
Normal file
@ -0,0 +1,29 @@
|
|||||||
|
#!/usr/bin/env python3
|
||||||
|
# -*- coding: utf-8 -*-
|
||||||
|
"""
|
||||||
|
Created on Fri Aug 18 19:05:04 2023
|
||||||
|
|
||||||
|
@author: astral
|
||||||
|
"""
|
||||||
|
|
||||||
|
from datetime import datetime
|
||||||
|
import numpy as np
|
||||||
|
from neuropercolation import Simulate2Layers
|
||||||
|
|
||||||
|
eps_space = np.linspace(0.005,0.5,100)
|
||||||
|
#eps_space = np.linspace(0.135,0.15,4)
|
||||||
|
|
||||||
|
dims=list(range(21,27,2))
|
||||||
|
for dim in [33]:
|
||||||
|
for eps in [0]:
|
||||||
|
eps = round(eps,3)
|
||||||
|
sim = Simulate2Layers(dim,
|
||||||
|
eps,
|
||||||
|
steps=5000,
|
||||||
|
draw='pygame',
|
||||||
|
save='simple',
|
||||||
|
path=f'/cloud/Public/_data/neuropercolation/2lay/steps=500000_rising/dim={dim:02}/',
|
||||||
|
rising=True,
|
||||||
|
fps=60,
|
||||||
|
)
|
||||||
|
print(f'Done eps={eps:.3f} with dim={dim} at {datetime.now()}')
|
@ -19,7 +19,7 @@ eps_space = np.linspace(0.005,0.5,100)
|
|||||||
#eps_space = np.linspace(0.135,0.15,4)
|
#eps_space = np.linspace(0.135,0.15,4)
|
||||||
|
|
||||||
stp = 1000100
|
stp = 1000100
|
||||||
dims = range(9,10)
|
dims = range(25,26)
|
||||||
batches = 1
|
batches = 1
|
||||||
|
|
||||||
path = f'/cloud/Public/_data/neuropercolation/4lay/cons=27-knight_steps=1000100_diares/dim=09/batch=0/'
|
path = f'/cloud/Public/_data/neuropercolation/4lay/cons=27-knight_steps=1000100_diares/dim=09/batch=0/'
|
||||||
@ -40,7 +40,7 @@ for dim in dims:
|
|||||||
for batch in range(max_bat, max_bat+batches):
|
for batch in range(max_bat, max_bat+batches):
|
||||||
savepath = dimpath + f'batch={batch}'
|
savepath = dimpath + f'batch={batch}'
|
||||||
new_folder(savepath)
|
new_folder(savepath)
|
||||||
for eps in [0.3]:#list(eps_space[61::2]):
|
for eps in [0.05]:#list(eps_space[61::2]):
|
||||||
eps = round(eps,3)
|
eps = round(eps,3)
|
||||||
initstate = [[0,0],[0,0]]
|
initstate = [[0,0],[0,0]]
|
||||||
sim = Simulate4Layers(dim,
|
sim = Simulate4Layers(dim,
|
||||||
@ -49,10 +49,10 @@ for dim in dims:
|
|||||||
init=initstate,
|
init=initstate,
|
||||||
steps=stp,
|
steps=stp,
|
||||||
noeffect=-1,
|
noeffect=-1,
|
||||||
#fps=20,
|
fps=60,
|
||||||
draw=None,
|
draw='pygame',
|
||||||
res=6,
|
res=10,
|
||||||
save='all',
|
save=None,
|
||||||
path=path,
|
path=path,
|
||||||
)
|
)
|
||||||
print(f'Done eps={eps:.3f} with dim={dim} at {datetime.now()}')
|
print(f'Done eps={eps:.3f} with dim={dim} at {datetime.now()}')
|
@ -248,6 +248,7 @@ class Simulate2Layers:
|
|||||||
save=None,
|
save=None,
|
||||||
path='/cloud/Public/_data/neuropercolation/test/',
|
path='/cloud/Public/_data/neuropercolation/test/',
|
||||||
state_to_color_cb=None,
|
state_to_color_cb=None,
|
||||||
|
rising=False,
|
||||||
*args, **kwargs):
|
*args, **kwargs):
|
||||||
"""
|
"""
|
||||||
Creates a window to render a 2D CellularAutomaton.
|
Creates a window to render a 2D CellularAutomaton.
|
||||||
@ -275,6 +276,7 @@ class Simulate2Layers:
|
|||||||
self.__state_list = []
|
self.__state_list = []
|
||||||
self.__activation_list = []
|
self.__activation_list = []
|
||||||
self.__channel_list = []
|
self.__channel_list = []
|
||||||
|
self.__rising = rising
|
||||||
self.run(evolutions_per_second=fps, last_evolution_step=steps)
|
self.run(evolutions_per_second=fps, last_evolution_step=steps)
|
||||||
|
|
||||||
def run(self,
|
def run(self,
|
||||||
@ -293,6 +295,9 @@ class Simulate2Layers:
|
|||||||
while self.__active and self._not_at_the_end(last_evolution_step):
|
while self.__active and self._not_at_the_end(last_evolution_step):
|
||||||
time_ca_start = time.time()
|
time_ca_start = time.time()
|
||||||
self._cellular_automaton.evolve(evolutions_per_draw)
|
self._cellular_automaton.evolve(evolutions_per_draw)
|
||||||
|
if self.__rising:
|
||||||
|
self._cellular_automaton.epsilon = self._cellular_automaton.evolution_step/last_evolution_step*0.5
|
||||||
|
|
||||||
self._track()
|
self._track()
|
||||||
if self.__draw_engine is not None:
|
if self.__draw_engine is not None:
|
||||||
time_ca_end = time.time()
|
time_ca_end = time.time()
|
||||||
|
Loading…
Reference in New Issue
Block a user